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United States Patent |
5,063,417
|
Hopfield
|
November 5, 1991
|
Molecular shift register based on electron transfer
Abstract
An electronic shift register memory (20) at the molecular level is
described. The memory elements are based on a chain of electron transfer
molecules (22) and the information is shifted by photoinduced (26)
electron transfer reactions. The device of the invention integrates
designed electronic molecules onto a VLSI substrate (36), providing an
example of a "molecular electronic device" which may be fabricated.
Inventors:
|
Hopfield; John J. (Pasadena, CA)
|
Assignee:
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California Institute of Technology (Pasadena, CA)
|
Appl. No.:
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221021 |
Filed:
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July 18, 1988 |
Current U.S. Class: |
257/40; 257/431; 257/E51.023; 257/E51.041; 257/E51.044; 377/64; 706/40 |
Intern'l Class: |
H01L 029/28 |
Field of Search: |
357/8,30 R,4
365/106,107,112
377/57,64,80
350/354
|
References Cited
U.S. Patent Documents
3953874 | Apr., 1976 | Aviram et al. | 357/8.
|
4574161 | Mar., 1986 | Marks | 357/8.
|
Other References
Moore, T. A. et al., "Photodriven Charge Separation . . . " Nature, vol.
307, pp. 630-632 (Feb. 16, 1984).
Streetman, B., Solid State Electronic Devices, 1972, Prentice-Hall, pp.
362-364.
|
Primary Examiner: James; Andrew J.
Assistant Examiner: Crane; Sara W.
Attorney, Agent or Firm: Benman & Collins
Goverment Interests
ORIGIN OF INVENTION
The present invention was made in the course of work performed under
Contract No. N000-14-87-K-0377 awarded by the Office of Naval Research.
Claims
What is claimed is:
1. An electronic shift register comprising (a) a plurality of molecular
devices formed on a semiconductor substrate which also supports a VLSI
circuit, to which said molecular devices are electrically and logically
connected, said molecular devices comprising a polymer made up of a
plurality of monomeric repeat units, each monomeric repeat unit comprising
at least three different monomers, with at least one monomer characterized
by an electron energy level having a ground state and an upper state to
which electrons may be excited and at least one of the remaining monomers
characterized by an electron energy level having a ground state only to
permit movement of an electron in a predetermined direction, and (b)
pulsed light means for exciting an electron to said upper state when light
is one and for permitting said electron to decay to a ground state of an
adjacent monomer when light is off.
2. The shift register of claim 1 wherein an electron is excited to said
upper state by electromagnetic radiation.
3. The shift register of claim 2 wherein said electron is excited by light.
4. The shift register of claim 3 wherein said light is provided by a laser
pulse.
5. The shift register of claim 1 wherein said molecular devices comprising
a polymer made up of a plurality of monomeric repeat units, each monomeric
repeat unit comprising at least three different monomers, two of which
have two different energy levels, each requiring different wavelengths of
electromagnetic radiation to excite them such that two separate events are
required to move electrons forward to the next repeat unit, and the
remaining monomers characterized by an electron energy level having a
ground state.
6. The shift register of claim 5 wherein said electron is excited by light.
7. The shift register of claim 6 wherein said light is provided by a laser
pulse.
8. An electronic shift register comprising (a) a plurality of molecular
devices formed on a semiconductor substrate which also supports a VLSI
circuit, to which said molecular devices are electrically and logically
connected, said molecular devices comprising a polymer made up of a
plurality of monomeric repeat units, each monomeric repeat unit comprising
at least three different monomers, with one monomer characterized by an
electron energy level having a ground state and an upper state to which
electrons may be excited and the remaining monomers characterized by an
electron energy level having a ground state only to permit movement of an
electron in a predetermined direction, and (b) pulsed light means for
exciting an electron to said upper state when light is on and for
permitting said electron to decay to a ground state of an adjacent monomer
when light is off.
9. The shift register of claim 8 wherein an electron is excited to said
upper state by light.
10. The shift register of claim 9 wherein said light is provided by a laser
pulse.
11. The shift register of claim 8 wherein said repeat unit comprises a
donor monomer, at least one intermediate monomer, and an acceptor monomer.
12. A molecular circuit for a shift register comprising a plurality of
substantially parallel polymer chains, each polymer chain of the same
length as the other polymer chains and comprising a plurality of repeat
monomeric units, each monomeric repeat unit comprising at least three
different monomers, with at least one monomer characterized by an electron
energy level having a ground state and an upper state to which electrons
may be excited and the remaining monomers characterized by an electron
energy level having a ground state, said molecular circuit adapted to be
responsive to pulsed light for exciting an electron to said upper state
when light is on and for permitting said electron to decay to a ground
state of an adjacent monomer when light is off.
13. The molecular circuit of claim 12 wherein an electron is excited to
said upper state by light.
14. The molecular circuit of claim 13 wherein said light is provided by a
laser pulse.
15. The molecular circuit of claim 12 wherein said repeat unit comprises a
donor monomer, at least one intermediate monomer, and an acceptor monomer.
16. The molecular circuit of claim 12 further comprising a conductive
source electrode to which one end of each polymer chain is attached and a
conductive receiving electrode to which the other end of each polymer
chain is attached.
17. The molecular circuit of claim 12 wherein one of said monomers is
characterized by an electron energy level having a ground state and an
upper state to which electrons may be excited.
18. The molecular circuit of claim 12 wherein two of said monomers are
characterized by an electron energy level having a ground state and an
upper state to which electrons may be excited, the difference between said
ground state and said upper state being different for each monomer such
that two wavelengths of light are required, one to excite an electron in
one monomer and the other to excite an electron in the other monomer,
thereby requiring two separate events to move an electron forward by one
repeat unit.
19. A method of storing and transferring information in a shift register
comprising a plurality of molecular devices on a semiconductor substrate
which also supports a VLSI circuit, to which said molecular devices are
electrically and logically connected, said molecular devices each
comprising a plurality of polymeric strands, each polymeric strand made up
of a plurality of monomeric repeat units, each monomeric repeat unit
comprising at least three different monomers, with one monomer
characterized by an electron energy level having a ground state and an
upper state to which electrons may be excited and the remaining monomers
characterized by an electron energy level having a ground state, one end
of each polymeric strand attached to a conductive source electrode, and
the opposite end of each polymeric strand attached to a conductive
receiving electrode, said method comprising:
(a) immersing said substrate in an electrolyte; and
(b) exciting the molecular devices with intense short pulses of light to
cause an electron to be excited to an upper state on one monomer and to
decay through successive monomers to the next monomer repeat unit, such
that one pulse of light moves an electron from one repeat unit to the
next.
20. A method of storing and transferring information in a shift register
comprising a plurality of molecular devices on a semiconductor substrate
which also supports a VLSI circuit, to which said molecular devices are
electrically and logically connected, said molecular devices each
comprising a plurality of polymeric strands, each polymeric strand made up
of a plurality of monomeric repeat units, each monomeric repeat unit
comprising at least three different monomers, with two monomers
characterized by an electron energy level having a ground state and an
upper state to which electrons may be excited, the difference between said
ground state and said upper state being different for said two monomers,
and the remaining monomers characterized by an electron energy level
having a ground state, one end of each polymeric strand attached to a
conductive source electrode, and the opposite end of each polymeric strand
attached to a conductive receiving electrode, said method comprising:
(a) immersing said substrate in an electrolyte; and
(b) exciting the molecular devices with intense pulses of light of
alternating wavelengths to cause an electron to be excited to an upper
state in a first monomer, then to cause an electron to be excited to an
upper state in a second monomer and to decay through successive monomers
to the next monomer repeat unit, such that two alternating pulses of light
of different wavelengths move an electron from one repeat unit to the
next.
Description
TECHNICAL FIELD
The present invention relates to shift registers, and, more particularly,
to shift registers comprising molecules and employing an electron transfer
mechanism.
BACKGROUND ART
Man-made computing devices at the molecular level have been described in
the prior art. In the prior art, the basic computing elements are
individual molecules or assemblies of active groups on the scale of 10 to
50 .ANG.. The "state" of such a molecular element is changed by altering
the conformation of a given molecule, or by the addition (or subtraction)
of an electron or a small chemical group.
There are several chief motivating ideas behind this literature. First,
since molecular computation takes place (molecular biology is really a
form of computation at the molecular level), it might be possible to build
"electronic" or non-biological computational devices at the molecular
level. Second, at the molecular level, one can understand how to build
"p-n junctions", "photo-junctions", "wires", and even "field-effect
transistors"; thus, all the essential elements of VLSI (very large scale
integration) technology appear to be present on the molecular scale.
Third, both the realities of molecular biology and the theory of
computation explain how to do essentially error-free computation with
error-prone or erroneously constructed devices. Thus, the inevitable
errors of construction, and the "noise" and errors which will be present
when the size of computing energies is decreased towards .apprxeq.50 kT
per decision (instead of the present .apprxeq.106.sup.6 kT per decision),
need not in principle cause errors in the overall computation done by such
devices.
These ideas suggest building a molecularly based chip having a device
density thousands of times larger than conventional VLSI (very large scale
integrated) chips. However, the absence of specific and detailed
suggestions for device structure and function has led to justified
pessimism about this field.
DISCLOSURE OF INVENTION
In accordance with the invention, a molecular device shift register,
employing electron transfer mechanism, is provided. The electronic shift
register comprises a plurality of molecular devices formed on a
semiconductor substrate which also supports a VLSI circuit, to which the
molecular devices are electrically and logically connected. The molecular
devices comprise a polymer made up of a plurality of monomeric repeat
units, with each monomeric repeat unit comprising at least three different
monomers. One of the monomers in each repeat unit is characterized by an
electron energy level having a ground state and an upper state to which
electrons may be excited, while the remaining monomers in each repeat unit
are characterized by an electron energy level having a ground state.
Also in accordance with the invention, a molecular circuit for a shift
register comprises a plurality of polymer chains. Each polymer chain is of
the same length as the other polymer chains and each polymer chain
comprises a plurality of repeat monomeric units, as defined above.
The shift register is immersed in an electrolyte. Exposure of the shift
register to intense short pulses of light cause electrons to move from one
repeat unit to the next unit.
The shift register of the invention has a memory density of 100 to 1,000
times that obtainable with present VLSI technology.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1a is a schematic diagram of a shift register of the prior art;
FIG. 1b is a schematic diagram of an electronic shift register of the prior
art;
FIG. 2a depicts schematically an example of a polymer suitably employed in
the invention, using a three-monomer repeat unit;
FIG. 2b depicts the one-electron energy levels of each monomeric unit;
FIGS. 3a and 3b show two strategies for constructing a shift register from
a chain of electron transfer active species;
FIG. 4 is a schematic representation of a molecular device in accordance
with the invention;
FIG. 5a depicts schematically simple branching of a polymer structure used
to construct the molecular device of the invention to achieve a degree of
amplification;
FIG. 5b depicts schematically complex branching of the polymer structure to
achieve a high degree of amplification;
FIG. 6 is an example of an electron transfer polymer suitable in the
practice of the invention;
FIG. 7a is another example of an electron transfer suitable in the practice
of the invention; and
FIG. 7b is an energy level scheme for the polymer of FIG. 7a.
BEST MODES FOR CARRYING OUT THE INVENTION
A shift register 10 is a form of memory. In concept, it consists of a set
of memory cells 12 connected in a line (FIG. 1a). Each cell stores one bit
of information. During each clock cycle, the contents of each cell is
shifted to the next register to the right. The first register 1 receives a
new bit of information to be stored, while the bit which was in the last
register n is transferred to the external circuit.
Electronic shift registers 10' generally involve two information storage
sites (12a, 12b) in a single cell 12' (FIG. 1b). Toward the end of a clock
cycle, the state of the right half (.beta..sub.i) of each cell is the
information stored. The early part of the next clock copies the bit in
.beta..sub.i of each cell is the information stored. The early part of the
next clock cycle copies the bit in .beta..sub.i into .alpha..sub.i+1, the
left hand half of the next cell. The latter part of the clock cycle moves
the bit from each .alpha..sub.i into .beta..sub.i. By separating the
operation into two parts, reliable copies of the information can be copied
without confusion. Electronic shift registers 10' are in commercial use as
circuit elements for a variety of time-delay and information storage uses.
Magnetic bubble memories are a form of shift register.
In accordance with the invention, a physical hybrid, comprising a plurality
of molecular devices (described below) and a silicon VLSI-style circuit,
on which the molecular devices are built, is provided. The silicon circuit
provides the means of making electronic and logical contact, with a
molecular structure comprising the molecular devices added thereto. The
base silicon chip has various metal and oxide parts exposed, and can be
fabricated with 1 .mu.m-scale lithography. Appropriate surface treatments
with appropriately designed molecular solutions and electrochemistry can
generate a functional chip in which the dominant computation is done by
the added molecular devices.
Employing a physical hybrid between the device of the invention and a
VLSI-style circuit poses a number of potential problems. These include (1)
the means of delivering the energy needed for the computation to the
molecules, (2) delivery of the clock signal to the device, (3) fabrication
of the molecular device, (4) communicating the molecular information with
the micrometer size features of the chip, and (5) dealing with errors.
All of the foregoing problems may be addressed by using molecular electron
transfer reactions as the fundamental computing element. A molecular
electronic shift register 20 can be made as in FIG. 2.
.alpha..beta..gamma..alpha..beta..gamma..alpha..beta..gamma. polymer 22 is
prepared, as shown in FIG. 2a. FIG. 2b shows the one-electron levels of
the units .alpha., .beta., .gamma., .alpha., .beta., -.gamma., . . . For
operational purposes, molecular subunits .beta.and .gamma. have no
relevant excited states, and are represented by single energy levels. The
units .alpha. have two energy levels: a ground state and an upper state to
which they can be excited by light.
Each polymer chain 22 comprises a plurality of monomeric repeat units 24,
each monomeric repeat unit comprising at least three monomers. In FIG. 2a,
three such monomers, .alpha., .beta., and .gamma. are shown. The first
monomer in the unit (.alpha.) is called the donor, while the last monomer
in the unit (.gamma.) is called the acceptor. In between, there may be one
or more intermediate monomers (.beta.).
Let the system initially be partially reduced, with electrons in the ground
state of, for example, units .alpha..sub.2 and .alpha..sub.3, but not in
.alpha..sub.1 or .alpha..sub.4. Assume for the moment that the thermal
transition rates for uphill electronic transitions are negligible, and
that .alpha. units are far enough apart that direct transfer of electrons
between different .alpha. units is "impossible". In this case, the
electronic state (.alpha..sub.1)(.alpha..sub.2).sup.-
(.alpha..sub.3).sup.- (.alpha..sub.4), is stable, and can be thought of as
a stored bit sequence 0110.
Next, expose the polymer to a short intense burst of light 26. If the
transitions shown by the solid arrows are much faster than the relevant
competing transitions shown by the dashed arrows, each electron (for
example starting on unit 3) will go (.alpha..sub.3).sup.-
.fwdarw.(.alpha..sub.3.sup.-).sup.* .fwdarw.(.beta..sub.3).sup.-
.fwdarw.(.gamma..sub.3).sup.- .fwdarw.(.alpha..sub.4).sup.-, and will thus
be moved one unit to the right by the light flash, as seen, for example,
in FIG. 3a. Such a polymer forms a molecular shift register, with a single
electron representing a stored bit.
Every synchronous chip has two global needs, a power supply and a system
clock. The configuration of the invention preferably employs periodic
pulses of light, the same everywhere on the chip, to supply these global
quantities. At the same time, the optical system required is very simple
in that no spatial resolution is required. This is an adequate solution to
the first two design problems.
The "logic" of this memory is described by the topology of a line.
Information is simply passed along without branching. This is the most
elementary logical structure conceivable, and an unbranched polymer
structure is a physical structure adequate to implement this logic. Making
unbranched polymers comprising a given number of monomer units is a solved
problem for both polypeptides and polynucleotides. It is even possible to
specify the order of various monomer subunits, as in the case of synthetic
proteins. The manufacture of a repeating polymer n units in length, with
special attachment groups "start" and "finish" at the two ends, can thus
be viewed as a problem which can be solved by modern approaches to
specific polymer construction. Thus, difficulty (3) can be circumvented
for a circuit as simple as a shift register.
Molecular electron transfer reactions are desirable because they involve no
bond formation or breakage, are reversible, have tunable rates, have an
intrinsic directionality, and a natural means of connecting the clock with
the energy source (i.e., a light source). FIG. 3 shows two strategies for
constructing a shift register from a chain of electron transfer active
species. These strategies utilize the polymer consisting of three
molecular groups per repeat unit described above. A "1" (or "0") is
written by reducing (or not reducing) the first repeat unit in the chain
which would not be in contact with an electrode. Exposing the chain to
short intense bursts of light shifts the written state one repeat unit to
the right, provided that the processes indicated with solid arrows are
much faster than their competing processes indicated with dashed arrows.
The potential of the electrode determines whether a 1 or 0 is written into
the shift register during a given light flash. On the three repeat units
shown in FIG. 3, the charge state represents the string "010". This design
uses periodic light pulses to both provide the power and to be the
synchronizing clock signal. Electrons are collected at an electrode (which
is also the gate of a transistor) at the terminus of the chain.
In FIG. 3a, three repeat units in an electron transfer shift register
scheme are shown, where the electron shift is initiated by excitation of
the donor (.alpha.). The presence of a 1 in the second cell is represented
by the presence of the electron (small up arrow). The dotted line
represents excitation of the donor by light. Solid lines show the transfer
reactions which shift the electron one unit down the chain following
photoexcitation. Back reactions which decrease the efficiency of the
device are shown with dashed arrows. The relative energies of the orbitals
are indicated.
The generic requirements for proper function in systems like the one in
FIG. 3a include (1) forward transfer from the excited donor must be much
faster than the corresponding radiative plus non-radiative decay to the
donor ground state (k.sub.1 <<k.sub.d); (2) all forward transfers must be
faster than reverse transfers (k.sub.2 >>k.sub.-1 and k.sub.3 >>k.sub.-2);
(3) electron transfer from the excited donor on the site to the right
(k.sub.1) must be much faster than the recombination rate (k.sub.-2) to
avoid a bottleneck at the connection between cells. (Similar systems with
more intermediate states might also be used.)
The intermediate serves the vital function of allowing a first extremely
fast charge transfer to compete with unproductive donor excited state
decay. The residence of the electron at the intermediate prevents the
confusion of the electron "bits" in adjacent cells. This intermediate also
provides a large distance between the acceptor and donor states within a
single repeat unit. Since electron transfer reactions decay approximately
exponentially with distance, intermediates are essential for efficient
charge transfer over long distances.
The intermediate electronic state is chosen with properties such that it
does not provide a thermodynamically allowed reverse electron transfer
reaction to occur. "Intermediates" which do not provide real reduced
intermediate states, but serve to increase the electronic coupling between
two other species may also prove useful.
Implicit in this discussion is the need for the clock cycle time to be long
compared to the time required to transfer an electron from donor to donor.
Also, the duration of the light pulse must be short enough that the
possibility of charge shifts longer than one repeat unit are eliminated.
In FIG. 3b, an example is shown where the intermediate (.beta.) is excited
on every unit of the chain every clock cycle. Units which are written with
a "0" simply relax back to the ground state via reactions k.sub.1 and
k.sub.-1. Proper shifting of the "1", written in the central cell in this
example, follows excitation, provided k.sub.2 >>k.sub.-1 and k.sub.-1
>>k.sub.3. Transfer from .alpha. to .beta. is only energetically allowed
when .alpha. is doubly occupied. If the light pulse is long (but shorter
than 1/k.sub.3), each monomer in state "1" may have several chances to
form the charge separated state.
Both schemes depicted in FIGS. 3a and 3b could also be equivalently
implemented with chiefly filled orbitals in place of the chiefly empty
cases illustrated.
A molecular circuit 30, shown in FIG. 4, is assembled by first binding the
head end of about 5000 polymer chains 22, each exactly 600 polymer units
long, (600 being a typical value) to one edge of a metal (or doped
semiconductor) conducting source electrode 32. This can be done by
activating one such edge by a deposition using directional shadowing, and
then using the activated area as an electrode to form a covalent bond with
a group such as a silal at the head end of the polymer chain. In a similar
fashion, the tail of the exactly 600 unit polymer can be covalently linked
to an edge of a similarly conducting receiving electrode 34.
Such an assembly of repeat units 24 would provide chains 22 of 1.2 .mu.m
(distance measured along the backbone), assuming that each repeat unit is
20 .ANG.. If there are exactly 600 units 24 in each polymer 22, the
precision of manufacturing is absolute, since the electrons move along the
polymer paths, even though errors in lithography will produce rough edges
of S and R, with local fluctuations of 1,000 .ANG..
Each such molecular circuit 30, comprising a plurality of polymeric strands
22, is supported on a substrate 36 and is connected to VLSI circuitry (not
shown) by input connection 38 and output connection 40.
In operation, the material would be immersed in electrolyte, such as salt
water or acetonitrile with TBAP (tetra-butyl ammonium perchlorate), and a
third (reference) electrochemical electrode placed in the solution. The
ionic strength of the electrolyte should be made adequate to keep the
Debye length to .apprxeq.20 .ANG.. Every clock cycle, the system is
excited by an intense short pulse of laser light.
If the source electrode 32 is kept high in potential, unit .alpha..sub.1,
which is next to the electrode, is oxidized. If electrode 32 is at low
potential however, unit .alpha..sub.1 will be reduced. A flash of light 26
will move an electron from .alpha..sub.1 .fwdarw..beta..sub.1
.fwdarw..tau..sub.1 .fwdarw..alpha..sub.2. If the potential is moved back
up, then .alpha..sub.1 will be re-oxidized, but unit .alpha..sub.2 will
stay reduced, since it is not in contact with electrode 32. In this
fashion, a "1" or "0" is written into the position .alpha..sub.2 in each
clock cycle. In each subsequent light pulse, the electrons marking the 1's
move one unit 24 to the right. After 600 light flashes, if a 1 was written
initially, all 5000 electrons (one from each of the polymers strands) will
be deposited on the receiving electrode 34. For example, electrode 34 may
be a 1 .mu.m.times.1.mu.m gate on a 100 .ANG. film of SiO.sub.2 above the
silicon transistor conductivity channel to be controlled.
The function of the conductivity in the supporting electrolyte is to
eliminate the image charge effect of other electrons near but not yet at
the electrode. The "cost" of this screening is that it results in shunt
capacitance for the receiving electrode. The number of necessary strands
22 is dictated by the amount of charge which must be delivered to a gate
in order to result in a good "1" or "0" being observed at the output of
the corresponding transistor. It has been estimated (when appropriately
scaled to 1 .mu.m lithography) that about 1000 electrons will suffice.
It would be possible to detect accurately as few as 100 electrons, but then
further stages of amplification would need to be built on the
semiconductor chip. In the configuration of the invention, the shunt
capacitance due to the electrolyte will be about 5 times the gate-channel
capacitance, so that about 5000 electrons will be required. This is why
5000 was chosen for the number of parallel chains 22. Fortunately, this
5000-fold redundancy is not a total waste. If, as is inevitable, a small
fraction of the chains have the wrong length, or an electron occasionally
does not move forward when struck by light, the parallelism of the 5000
chains 22 will preserve the information, since 5000 independent copies are
summed at electrode 34.
The most important single parameter in the molecular design is high
transfer efficiency. If the polymers 22 are 600 units long, in order that
most of the electrons arrive at the correct time, the transfer probability
per step must be at least 0.999. Of course, if the length of the strands
is decreased, or several electrons in a row are used to represent a bit,
this restriction could be reduced substantially. At the same time, less
information would be stored.
The light source must generate a short saturating flash of light 26 every
clock cycle. The pulse must be short in order that there is no possibility
of two transitions to the right in one clock cycle. To have a probability
.gtoreq.99.9% of exciting a given molecule, the flash of light must be
moderately strong. For molecules with a molar extinction coefficient of
10.sup.5, the pulse must represent an energy flux 20 millijoules/cm.sup.2.
The actual amount of energy which gets absorbed per clock cycle is still
not large.
Each clock cycle, the minimal energy absorption is 1.5.times.10.sup.15
joules/bit stored/clock cycle. Thus, a 1 cm.sup.2 chip storing 10.sup.9
bits and with a clock speed of 1 megacycle will only dissipate about 1.5
watts. The discrepancy between this and the otherwise expected
0.020.times.10.sup.6 =20 Kilowatts is due to the fact that a chip storing
10.sup.9 bits on 1 cm.sup.2 by these techniques is optically extremely
thin, and absorbs very little of the light striking it.
Photosynthetic bacteria have a reaction center which has evolved to have
properties very similar to those needed for a monomer of the chain. Such
reaction centers contain a sequence of aromatic groups:
______________________________________
.alpha.' .alpha. .beta. .gamma.
______________________________________
cytochrome
bacterial bacterial ubiquinone
chlorophyll pheophytin
______________________________________
which has a quantum yield for the .alpha.' to .gamma. photo-activated
.alpha. charge separation process greater than 95%. The yield has never
been measured directly with much precision. A rate of 8.times.10.sup.7
sec.sup.-1 has been determined for the reaction (.alpha..sup.+B-
.fwdarw..alpha..beta.) by using chemically modified reaction centers. The
rate of the electron transfer
.beta..sup.- .tau..fwdarw..beta..gamma..sup.-
is 7.times.10.sup.9 sec.sup.-1. The competition of these two rates is
believed to limit the quantum efficiency of the reaction center. Thus, one
would calculate the efficiency to be 98.9%. Note that the limiting feature
is the rate of transfer
.beta..sup.- .gamma..fwdarw..gamma..sup.-.beta.
If these two moieties were in closer proximity, this rate would be
increased substantially without altering other important aspects of the
problem. Thus, synthetic structure of the reaction-center type and having
quantum efficiencies >99% will certainly be possible.
While the reaction center is of an .alpha.,.alpha..beta..gamma.structure, a
3-unit monomer should be adequate for the task. Much is known about the
design and synthesis of such compounds and about the rate of electron
transfer in relevant rigid structures. A synthetic .alpha.'.alpha..beta.
trimer system has been synthesized, but relatively poorly characterized
from an electron transfer viewpoint. The conceptual variables are redox
energies, chromophore excitation energy, linker type and length, and
degree of vibronic coupling.
Major constraints in the design of an .alpha.-.beta.-.gamma. unit include
1) low vibronic coupling to decrease the rate of back reactions;
2) a rigid linking structure so that molecules are not likely to fold back
on themselves;
3) good covalent (perhaps unsaturated) linking pathways for fast transfers;
4) choice of .alpha.,.beta.,.gamma. such that dimerization of different
strands of inter-strand electron transfer is unlikely, for example,
charged side-groups, bulky hydrocarbon side-groups;
5) excellent resistance to photo-degradation, for example, phthallocyanins
rather than porphyrins;
6) appropriate redox levels and excited single and triplet levels;
7) monomers are to be used in polymer synthesis of long ordered chains.
This molecular design problem is certainly solvable, though not easy,
within the current framework of chemical synthesis and electron transfer
theory. For example, using an alternate route to such a synthesis based on
the present ability to synthesize define double-stranded DNA polymers, an
appropriate DNA sequence could then be used as a backbone on which to
graft .alpha.,.beta.,.gamma. units, which would attach at defined
locations on the (periodic) DNA structure.
Two examples of electron transfer polymers which may be suitable for use as
molecular shift registers are depicted in FIGS. 6 and 7a. The energy level
scheme for the polymer shown in FIG. 6 is the same as that depicted in
FIG. 3a. In the notation in FIG. 6 listed below the molecule, MP=a
metallo-porphyrin, where M=Mg, Zn, Cd, etc., .phi.=phenyl, Q.sub.1
=quinone, and Q.sub.2 =chloroquinone.
For the polymer shown in FIG. 7a, the energy level is illustrated in FIG.
7b. A null entry must be inserted between all "bits" for the scheme to
function properly. In FIG. 7a, bpy=bipyridine and R may comprise a
methylene link (--CH.sub.2 --), a phenyl link (C.sub.6 H.sub.4) or have a
value of zero (direct link from the nitrogen in the ring to the phenyl
ring in the next unit). In FIG. 7b, R=ruthenium (bipyridine), MV=methyl
viologen, and DMA=dimethyl aniline.
Consideration of this shift register focuses attention on several
significant aspects of molecular computation. For instance, while
molecularly based computation might reasonable promise computation
energies of about 50 kT/bit handled, the present chip design requires
about 5.times.10.sup.5 kT/bit handled. The shift register design herein
makes no progress in energy per bit handled.
The fundamental origin of this ineffectiveness is the unbranched structure
of the polymer. The need for 5000 electrons at the end necessitates 5,000
strands 22 everywhere. But suppose a molecular branch unit could be
constructed, so that one electron arriving at the fork could generate two
electrons and a hole traveling on separate strands as indicated in FIG.
5a. With such a unit, a tree-like structure like that in FIG. 4b can be
made which could amplify one electron into 1,000 in 10 branchings. Ten
polymer strands, each with a tree at the end, to make 1,000 copies of the
charge would then be sufficient. (The electrons would need to be collected
at one electrode, and the corresponding holes at another.) This would
reduce the energy per bit down to 1,000 kT.
The linear polymer shift register of the invention does the almost trivial
job of moving binary bits. The next more complex job in computation is to
copy information, which is what the forked molecular polymer structure of
FIG. 5 does. Forks seem essential to any larger potential for such
molecular devices. There is no present molecular scheme which has
demonstrated this fork or copy property, but there are several conceptual
approaches to this problem. Some are based on detailed two-electron
transfers in particular systems; and others on using an electron to
control a tunneling matrix element (analogous to a gate in a field effect
transistor).
If digital computation is to be carried out at a molecular level, a "bit"
must have a physical representation. Possibilities include representing
1/0 by the presence/absence of an electron, an electronic excited state,
an exciton, a soliton, a choice of molecular conformations, a spin, etc.
The choice made here of the electron as a bit has the advantage that it
interfaces in a natural way with reading and writing by electrical
circuits. In addition, the conservation of electrons tends to keep bits
from being spontaneously created or destroyed. There are also
well-developed methods of moving electron "bits". The absence of a
well-developed "copy" procedure is a weakness shared by all the other
possible "bit" representations.
It may be a simplification to use light pulses of two different wavelengths
for driving such a system. The usual electronic shift register discussed
earlier separates the information transfer into two separate steps. This
could be done in a molecular shift register as well. A system designed so
that .alpha..fwdarw..beta. is driven by a wavelength .lambda..sub.1, while
.beta..fwdarw..gamma. is driven by .lambda..sub.2 would have the desired
property. In use, pulses of .lambda..sub.1 and .lambda..sub.2 would
alternate. The advantages of this scheme is that the light pulses need not
be short compared to electron transfer times, since there can be a
movement of only one monomer unit per clock cycle regardless of how long
the pulses last. Both the demands on the laser and the problem of
multi-photon effects are simplified by such a scheme.
Light, which includes that portion of the electromagnetic spectrum from
near-IR to visible and near-UV, is one answer to the clock and power
supply problem. Using light, the fabrication problem for a real device
appears to be within what is understood of chemistry, VLSI, and physics.
Light is quite possibly not the only answer, however. As others have
noted, diffusing energetic molecules, playing the role of ATP (adenosine
triphosphate), could in principle, be a much better power supply.
Molecular wires might solve both the clock and/or power supply problems.
But such solutions involve technical problems for which detailed solutions
are at present lacking.
A shift .alpha..beta..gamma.polymer 22 with high efficiency would be
interesting in its own right. The general question of light-driven shift
polymers can be investigated with far shorter oligomers tethered at only
one end, and without the need for microfabrication.
The materials science and chemical synthesis questions raised in such
schemes are also of interest for more conventional electronics. For
example, much simpler electron transfer polymers could be made to serve as
molecular wires over short distances in conventional VLSI without the need
for light as a driving source. Short-range self-wiring using such
molecules might replace certain metallization or polysilicon layers. This
would be particularly attractive if a class of specific surface-to-polymer
end bindings (through which electrons could be transferred) were
developed. Such an approach relates also to neural network chip
architectures, where the connectivity is complex, where wiring faults can
be tolerated, and for which connections of having a large resistance can
be a central part of a computational circuit. For example, a single strand
of half-reduced .alpha..sub.1.sup.- .alpha..sub.2.sup.-
.alpha..sub.3.sup.- .alpha..sub.4 . . . polymer 4,000 units long and
having an internal electron transfer rate .alpha..sub.i
.revreaction..alpha..sub.i+1 of f sec.sup.-1 has an electrical resistance
of about 10.sup.21 /f ohms. Since f can be made as large as 10.sup.11 for
hopping transfers between very nearby localized sites, a single strand a
few micrometers long can have a resistance as low as 10.sup.10 ohms. A
single such molecular strand has sufficient conductance to discharge a
small VLSI floating gate in a millisecond.
INDUSTRIAL APPLICABILITY
The molecular shift register of the invention is expected to find use as a
hybrid in conjunction with VLSI circuits to provide considerably greater
information density than presently available.
Thus, a molecular shift register based on electron transfer has been
disclosed. It will be appreciated by those skilled in the art that various
changes and modifications of an obvious nature may be made without
departing from the spirit and scope of the invention, and all such changes
and modifications are considered to fall within the scope of the invention
as defined by the appended claims.
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